Researchers with a continuum-mechanical background typically use a multi-phasic and multi-component modelling approach for materials with a saturated porous microstructure. Therefore, the mechanical behaviour is considered in a continuummechanical manner and solved using the finite-element method (FEM). The developed models need to be complex enough to capture the relevant properties of the considered materials, what often results in expensive simulations with a very large number of degrees of freedom (DOF). The aim of the present contribution is to reduce the computing time of these simulations through model-reduction methods, while the accuracy of the solution needs to be maintained. Therefore, the method of properorthogonal decomposition (POD) for linear problems and the discrete-empirical-interpolation method (DEIM) in combination with the POD method (POD-DEIM) for nonlinear problems are investigated.Using the POD method, a given data set is approximated with a low-dimensional subspace. To generate this data set, the vector of unknowns of the FE simulation is stored in a pre-computation in the full (unreduced) system in each time-step (so-called "snapshots" of the system). Dealing with porous-media problems, the primary variables are the solid displacement, the pore pressure and, depending on the particular problem, other primary variables. Following this, the primary variables have entries with very huge differences in their absolute values. As a result, non-negligible rounding errors may occur when applying the POD method. To overcome this problems, modifications of the classical POD method need to be performed for such problems. The present contribution discusses this issue and presents results for the reduced simulations of porous media.
In the context of clinical treatment, reliable models of biological materials can provide further information of the occurring processes. For this purpose, the prediction of various simulation scenarios or real-time simulations is desirable. A broad variety of biological materials, such as intervertebral discs or skeletal muscles, exhibit a porous microstructure and are conveniently simulated using a macroscopic continuum-mechanical modelling approach. Therefore, the complex inner structure is regarded in a multi-phasic manner using the Theory of Porous Media (TPM). The solution of the descriptive set of coupled partial differential equations (PDE) is approximated with the finite-element (FE) method.In the context of FE simulations, computing time and numerical effort is an important issue because the number of degrees of freedom (DOF) of such coupled problems can become very large. To reduce the numerical effort, the method of proper orthogonal decomposition (POD) is applied in combination with the discrete-empirical interpolation method (DEIM). Using the POD method, representative state variables (so-called snapshots) are stored in pre-computations using the initial full system and are approximated with a low-dimensional subspace. Additionally, snapshots of the nonlinear terms of the differential equation are stored to approximate the nonlinearities using the DEIM. Dealing with porous-media problems in biomechanical applications, the primary variables (such as the solid displacement or the pore pressure) exhibit a different temporal behaviour. In order to take this into account, the snapshots are divided in separated parts for each primary variable. Modelling approachDue to the complex structure of porous biological materials, a macroscopic continuum-mechanical modelling is applied. Here, the developed constitutive model is based on the well-founded TPM, combining the Theory of Mixtures (TM) with the concept of volume fractions, see [2]. The balance relations are derived in analogy to the balance relations of single-phasic continuum mechanics but allow for interactions between the constituents by so-called production terms. After inserting constitutive assumptions, the balance relations are transferred to weak formulations. The system of weak formulations is then spatially discretised using mixed finite elements and solved in a monolithic manner viawith the system matrix M (u), the system vector k(u) and the vector f (t) consisting of the Neumann boundary conditions. The vector u of unknowns contains the nodal unknowns of each primary variable and the vectoru their time derivatives. Model-reduction methodsThe basic idea of projection-based model-reduction methods is to transform a high-dimensional system to a low-dimensional subspace to minimise the numerical effort. Using the POD method to compute the subspace matrix, the values of the vectors u i of unknowns (at times t i , i = 1, ..., m) need to be stored in a snapshot matrix U = [u 1 u 2 ... u m ] during pre-computations using the initial full system, see...
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